Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Dynamik und Statistische Physik Donnerstag<br />
presence of shear flow. Generalizing the approach of [2], ferrofluid droplets<br />
are modeled as deformable and orientable ellipsoids of revolution.<br />
The combined effects of a magnetic field and a shear flow on the orientation<br />
and deformation of the droplets are studied. It is found that the<br />
hydrodynamic drag leads to a flow alignment of the droplet orientation.<br />
Predictions for the alignment angle as a function of the applied field are<br />
presented. Some comparisons to experimental data [3] in the absence of<br />
shear are made.<br />
[1] E. Blums, A. Cebers, M.M. Maiorov, Magnetic Fluids, deGruyter,<br />
Berlin 1997.<br />
[2] P. Ilg and M. Kröger, Phys. Rev. E 66, 021501-1 (2002)<br />
[3] A. Lebedev, A. Engel, K.I. Morozov and H. Bauke, New Journal of<br />
Physics 5, 57.1-57.20 (2003)<br />
DY 46.81 Do 16:00 Poster D<br />
The corkscrew instability in a nematic liquid crystal —<br />
•Alberto de Lozar, Wolfgang Schoepf, Lorenz Kramer, and<br />
Ingo Rehberg — Universitaet Bayreuth<br />
A liquid crystal with slightly positive dielectric anisotropy is investigated<br />
in the planar configuration. This system allows for competition<br />
between electroconvection and the homogeneous Frèedericksz transition,<br />
leading to a rather complicated bifurcation scenario. We report measurements<br />
of a novel instability leading to the ”corkscrew” pattern. This state<br />
is closely connected to the Frèedericksz state as it manifests itself as a regular<br />
modulation along a Frèedericksz domain wall, although its frequency<br />
dependence indicates that electroconvection must play a crucial role. It<br />
can be understood in terms of a pitchfork bifurcation from a straight<br />
domain wall. Quantitative characterization is performed in terms of amplitude,<br />
wavelenght and relaxation time. Its wavelenght is of the order of<br />
the probe thickness, while its ondulation amplitude is an order of magnitude<br />
smaller. The relaxation time is comparable to the one obtained for<br />
electroconvection.<br />
DY 46.82 Do 16:00 Poster D<br />
Magneto-rheological study in inverse magnetic fluids using<br />
polystyrene particles — •Saldivar-Guerrero Ruben 1 , Richte<br />
Reinhard 1 , Rehberg Ingo 1 , and Rodriguez-Fernandez Oliverio<br />
2 — 1 Universitaet Bayreuth, Experimentalphysik V — 2 Centro de<br />
Investigacion en Quimica Aplicada<br />
Ferrofluids are colloidal suspensions of magnetic nanoparticles, which<br />
change their behaviour under control of an external magnetic field. But<br />
when for example, they are mixed with polystyrene particles, they present<br />
another interesting properties. The magneto-rheological fluid (MRF) obtained<br />
in this way, can show a solid-fluid transition by an application<br />
of a moderate magnetic field similar to electro-rehological fluids (ERF)<br />
under a electric field. It excels ERF’s because only moderates currents<br />
instead of high voltages are necessary. We study the rheological influence<br />
of the diameter of the immersed polymer particle in MRF and the relation<br />
between the coupling parameter l and the yield point ty for different<br />
magnetic fields applied. The results show that the rheological properties<br />
are increased when the particle diameter increases in a constant magnetic<br />
field. Also we investigate structure formation in the fluid by video<br />
microscopy when a magnetic field is applied.<br />
DY 46.83 Do 16:00 Poster D<br />
Smectic and crystalline order in colloidal monolayers on periodic<br />
one-dimensional substrate potentials — •Jörg Baumgartl<br />
1 , Matthias Brunner 2 , and Clemens Bechinger 1 — 1 2.<br />
Physikalisches Institut, Universität Stuttgart, Pfaffenwaldring 57, 70550<br />
Stuttgart — 2 Fachbereich Physik, Universität Konstanz, 78457 Konstanz<br />
There is growing interest in the phase behavior of two-dimensional<br />
(2D) colloids in the presence of one-dimensional (1D) periodic substrate<br />
potentials. The phase behavior of such systems is determined by two factors:<br />
(i) the relative orientation between the 2D crystal and the periodic<br />
potential troughs which selects a set of Bragg planes running parallel to<br />
the troughs and (ii) the commensurability ratio p = a ′ /d of the spacing<br />
a ′ between these Bragg planes to the period d of the periodic potential.<br />
So far, only the phase behavior for p = 1 was investigated and the following<br />
phases were observed for increasing (non zero) potential strength:<br />
modulated liquid and light-induced crystal. For other commensurability<br />
ratios additional, more complex phases are predicted.<br />
We investigated experimentally the phase behavior for the case p = 2<br />
with the 1D periodic potential being created by two interfering laser<br />
beams. We observed for the first time the theoretically predicted intermediate<br />
phase between modulated liquid and light-induced crystal which<br />
is termed locked smectic. By analyzing the structure factor and the pair<br />
correlation function, this phase is characterized by liquid-like behavior<br />
along the potential troughs. In contrast to the modulated liquid the ordering<br />
perpendicular to the troughs is similar to the crystalline state,<br />
with particles occupying only each second trough.<br />
DY 46.84 Do 16:00 Poster D<br />
Commensurability effects of colloidal monolayers on hexagonally<br />
patterned substrates — •Stefan Bleil 1 , Matthias Brunner<br />
2 , and Clemens Bechinger 1 — 1 2. Physikalisches Institut, Universität<br />
Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart — 2 Fachbereich<br />
Physik, Universität Konstanz, 78457 Konstanz<br />
Colloidal suspensions are excellent model systems for investigations<br />
of phase transitions in two-dimensional (2D) systems. While most of<br />
the previous work concentrated on homogeneous substrates, much less<br />
is known about the phase behavior on patterned substrates although<br />
the latter closely resembles the behavior of atomic adsorbates on crystalline<br />
surfaces. In our experiments we mimic 2D patterned substrates<br />
for colloidal particles by the interference pattern of several laser beams<br />
which lead to triangular substrate potentials. We present results where<br />
the number density of charge stabilized colloidal particles was systematically<br />
varied. This allowed us to study the effect of the filling fraction<br />
η (i.e. the ratio between the number of colloidal particles and the number<br />
of substrate wells) on the observed structure of the colloidal system.<br />
Depending on the filling fraction we observe commensurate and incommensurate<br />
structures. We also compare our results with recent numerical<br />
simulations.<br />
DY 46.85 Do 16:00 Poster D<br />
Phasetransitions in Quantum fluids: PIMC - Studies — •Guido<br />
Günther and Peter Nielaba — Lehrstuhl für Theoretische Physik,<br />
Fachbereich Physik, Universität Konstanz, D-78457 Konstanz<br />
Exploiting path integral Monte Carlo methods we studied the behavior<br />
of the fluid phase of quantum mechanical hard sphere- and disk- systems.<br />
We focused on the superfluid phase transition of Bose systems<br />
analyzing, among other quantities, the superfluid fraction which in<br />
periodic boundary conditions is related to the winding number of the<br />
Trotter-chains [0].<br />
[0] E.L. Pollock, D.M. Ceperley; Phys. Rev. B 36, 8343 (1987)<br />
DY 46.86 Do 16:00 Poster D<br />
Microcanonical entropy of classical spin systems with a continuous<br />
symmetry — •Andreas Richter, Michel Pleimling,<br />
and Alfred Hüller — Institut für Theoretische Physik I, Universität<br />
Erlangen-Nürnberg, D-91058 Erlangen<br />
Critical phenomena of classical spin systems may be studied in many<br />
ways. In our approach we determine and analyse the microcanonical entropy<br />
S which is related to the density of states by S = kB ln Ω, where kB<br />
is the Boltzmann constant. Due to the huge amount of possible configurations<br />
it is in general impossible to calculate Ω exactly, even for systems<br />
of moderate size. The density of states can, however, be computed approximately<br />
from a numerical method using transition variables. Discrete<br />
classical systems, like the Ising or Potts model, were already studied with<br />
this method in the past [1,2]. We now extend this method to systems with<br />
continuous spins and apply it to the three-dimensional XY model. In addition,<br />
we discuss the determination of critical quantities directly from<br />
the numerically determined microcanonical entropy.<br />
[1] A. Hüller, M. Pleimling, Int. J. Mod. Phys. C 13, 947 (2002)<br />
[2] H. Behringer, J. Phys. A: Math. Gen 36, 8739 (2003)<br />
DY 46.87 Do 16:00 Poster D<br />
A Topological Rule-of-Thumb for Percolation Thresholds —<br />
•Richard Neher and Herbert Wagner — Sektion Physik, Universität<br />
München<br />
Randomly assembled structures exhibit a density driven percolation<br />
transition, beyond which an unbounded component is formed. Since properties<br />
of those structures change dramatically at the percolation threshold,<br />
its accurate knowlegde is important and various empirical formulas,<br />
predicting percolation thresholds, have been suggested. The mean Euler<br />
characteristic is a topological measure for such random sets and it has<br />
been suggested to use its zero crossing to estimate the threshold. In contrast<br />
to other formulas, this estimation does not rely on a fit to known<br />
thresholds.<br />
We further investigated this matter and found, that for a great variety